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JPS6098854A - Ac generator - Google Patents

Ac generator

Info

Publication number
JPS6098854A
JPS6098854A JP20715383A JP20715383A JPS6098854A JP S6098854 A JPS6098854 A JP S6098854A JP 20715383 A JP20715383 A JP 20715383A JP 20715383 A JP20715383 A JP 20715383A JP S6098854 A JPS6098854 A JP S6098854A
Authority
JP
Japan
Prior art keywords
magnetic pole
portions
pair
magnetic
rotor
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
JP20715383A
Other languages
Japanese (ja)
Other versions
JPH0564540B2 (en
Inventor
Arata Kusase
新 草瀬
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Denso Corp
Original Assignee
NipponDenso Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by NipponDenso Co Ltd filed Critical NipponDenso Co Ltd
Priority to JP20715383A priority Critical patent/JPS6098854A/en
Publication of JPS6098854A publication Critical patent/JPS6098854A/en
Publication of JPH0564540B2 publication Critical patent/JPH0564540B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02KDYNAMO-ELECTRIC MACHINES
    • H02K1/00Details of the magnetic circuit
    • H02K1/06Details of the magnetic circuit characterised by the shape, form or construction
    • H02K1/22Rotating parts of the magnetic circuit
    • H02K1/24Rotor cores with salient poles ; Variable reluctance rotors
    • H02K1/243Rotor cores with salient poles ; Variable reluctance rotors of the claw-pole type

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Synchronous Machinery (AREA)

Abstract

PURPOSE:To reduce the leakage magnetic flux from the end of a pole of a rotor to the opposed reverse pole of a disc by forming a pair of substantially chamfered portions radially of the pole disc. CONSTITUTION:A toothed portion 20 of a pole has a substantially arcuate-shaped end 21 including the prescribed radius. A skirt portion 22 of substantially trapezoidal shape is formed continuously to the end 21. A pair of chamfered portions 25 with the prescribed angle are formed at both sides of the skirt 22. A pair of chamfered portions 35 are formed radially on a magnetic disc 30 continued to the portion 25. Further, a collar 26 is formed along a rectilinear line for coupling the both ends of the bottom of the skirt 22 from the both ends of the end 21 at the front. The toothed portion 20 has a side 28.

Description

【発明の詳細な説明】 (本発明の利用分野) 本発明は交流発電機に関し、特に車両用三相交流発電機
の回転子の1NU(ボールコア)形状の改良に関づる。
DETAILED DESCRIPTION OF THE INVENTION (Field of Application of the Invention) The present invention relates to an alternating current generator, and particularly to an improvement in the 1NU (ball core) shape of a rotor of a three-phase alternating current generator for a vehicle.

(従来の問題点) 従来のボールコアは台形状の先端部を有し、このボール
コアの隣接W(か間において漏洩磁束が大きく励磁力の
割には大さな出力が出なかった。この点を改良するため
、例えば米国特許 第3.004.181号明細書に見るようにボールコア
外表面につば部を設け11極面積を増大させる一方でボ
ールコア内側を「そぎ」落し形状として対向異極間の磁
気抵抗を増加させ漏洩磁束を軽減させる方法があった。
(Conventional problems) The conventional ball core has a trapezoidal tip, and the leakage magnetic flux is large between the adjacent W (W) of this ball core, and a large output is not produced in relation to the excitation force. In order to improve this point, for example, as seen in U.S. Pat. No. 3,004,181, a flange is provided on the outer surface of the ball core to increase the area of the 11 poles, while the inner side of the ball core is "scraped" so that they face each other. There is a method to reduce leakage magnetic flux by increasing the magnetic resistance between different poles.

しかし、この方法のように単につば形状を設けるのみで
は台形状ボールコア側面の漏洩磁束は低減するものの、
台形状ボールコア先端部から対向ボールコアディスク部
(円板部)へと流れる漏洩磁束はっばなしボールコアの
場合以上に増大づるという欠点があり、全体としての漏
洩磁束軽減効果はほとんどないのが実状であった。
However, although simply providing a brim shape as in this method reduces the leakage magnetic flux on the side surface of the trapezoidal ball core,
The disadvantage is that the leakage magnetic flux flowing from the tip of the trapezoidal ball core to the opposing ball core disk section (disc section) increases more than in the case of a flat ball core, and there is almost no effect on reducing leakage magnetic flux as a whole. That was the actual situation.

(本発明の目的) 本発明は上記の問題点に鑑みてなされICものであり、
交流発電機の回転子磁極の側面からの漏洩磁束を低減す
ることおよびさらにその磁極先端部から対向ボールコア
ディスク部へ流れる漏洩磁束を低減り″ることを目的と
する。
(Object of the present invention) The present invention has been made in view of the above problems, and is an IC.
The purpose of this invention is to reduce the leakage magnetic flux from the side surfaces of the rotor magnetic poles of an alternator, and further to reduce the leakage magnetic flux flowing from the tips of the magnetic poles to the opposed ball core disk parts.

(本発明の構成) 本発明は一対の磁極円板部に設りられた複数個の磁極歯
部に所定の半径を有する円弧状先端部が形成されさらに
上記円板部の半径方向に一対の面取り部が形成されてな
る回転子を含む交流発電機である。更に、本発明は上記
の構成に加えて16極歯部が先端部から実質的にテーパ
状をなした裾野部とこの裾野部および先端部に関し−C
はぼ台形状をなした断面とを有り−る476成を持つ。
(Structure of the present invention) The present invention is characterized in that a plurality of magnetic pole teeth provided on a pair of magnetic pole disk portions are formed with arc-shaped tip portions having a predetermined radius, and further, a pair of magnetic pole tooth portions provided on a pair of magnetic pole disk portions are formed with arc-shaped tip portions having a predetermined radius. This is an alternator that includes a rotor with a chamfered portion. Furthermore, in addition to the above configuration, the present invention relates to a base portion in which the 16-pole tooth portion is substantially tapered from the tip portion, and this base portion and the tip portion.
It has a 476 configuration with a trapezoidal cross section.

本発明はさらに上記のすべての構成に加えて磁極歯部が
裾野815にその+Iづ1方向に泊って形成された別の
一対の面取り部を右する構成を持つ。
In addition to all of the above configurations, the present invention further has a configuration in which the magnetic pole teeth form another pair of chamfered portions formed on the skirt 815 in one direction, +I.

(従来の具体的問題魚) 以下、添付図面について説明する。第1図(a )およ
び(b’)は従来の交流発電機の回転子にお【ノる磁極
部分を示す。一対の磁極円板部1は対向配置され、各円
板部1(,1イの周辺に相互に隔置された複数個の磁極
歯部2を有している。各歯部2は円周方向につば部3を
形成し、−窓空間を隔て交互に反対極性で歯合状態にあ
る。歯部2の先端は台形状であり、角部4を右J゛る。
(Conventional specific problem fish) The attached drawings will be explained below. FIGS. 1(a) and 1(b') show the magnetic pole portions of the rotor of a conventional alternator. A pair of magnetic pole disk portions 1 are arranged to face each other, and have a plurality of magnetic pole tooth portions 2 spaced apart from each other around each disk portion 1 (, 1a). A flange 3 is formed in the direction, and they are alternately meshed with opposite polarity across a window space.The tips of the teeth 2 are trapezoidal and extend from the corner 4 to the right.

歯部2はさらに側面5およびテーバ状の底面6を有する
。第2図は従来の交流発電機の回転子おJ:び固定子部
分を示す。第2図においC17は固定子コイル、8は固
定子コア、9は回転子コイル、10は回転子シャフトで
ある。
The tooth 2 further has a side surface 5 and a tapered bottom surface 6. FIG. 2 shows the rotor and stator portions of a conventional alternator. In FIG. 2, C17 is a stator coil, 8 is a stator core, 9 is a rotor coil, and 10 is a rotor shaft.

第1図(a )、(11)おJ:び第2図の交流発電機
の回転子において、磁極歯部先端がら対向異極へと漏洩
する磁束φlb は従来のつば無しの台形磁極のもの以
上に増大し、この増大した漏洩磁束φゎ はつば付き形
状にして得られる磁極面積拡大による固定子・回転子!
!間の空隙パーミアンスのイ[(下という効果を減殺す
る。特に、負荷電流が流れていわゆる電(幾子反作用ア
ンペアターンが発生し増大すると、この空隙パーミアン
スはこれが従来のつば無し磁極のものよりも低いだけに
一層大きな減磁作用として効いてくる。しかし、一方で
界磁起磁力も高くこれに反抗するので大部分の磁束は回
転子の鉄部を通れなくなり固定子・回転子空間を流れる
。したがって、漏洩磁束φハ は著しく増大づるため磁
極面積拡大を目的としたつば形状は負荷電流が大きくな
ればなるほど空隙パーミアンスの低減という効果を希薄
としているばかりでなく、つば無しの台形磁極のものよ
りも逆にl1ii洩磁束を増大させるという結果となっ
ている。
In the alternator rotor shown in Figures 1 (a) and (11) and Figure 2, the magnetic flux φlb leaking from the tip of the magnetic pole teeth to the opposite pole is that of a conventional trapezoidal magnetic pole without a flange. This increased leakage magnetic flux φゎ is due to the enlarged magnetic pole area of the stator and rotor, which can be obtained by using the flange shape!
! In particular, when the load current flows and the so-called electromagnetic reaction ampere turns occur and increase, this air gap permeance will be lower than that of conventional brimless magnetic poles. However, since the field magnetomotive force is also high and opposes this, most of the magnetic flux cannot pass through the iron part of the rotor and flows through the stator/rotor space. , the leakage magnetic flux φ increases significantly, so the shape of the brim for the purpose of expanding the magnetic pole area not only becomes less effective in reducing air gap permeance as the load current increases, but also has a shape that is smaller than that of a trapezoidal magnetic pole without a brim. On the contrary, the result is that the l1ii leakage flux increases.

(本発明の一実施例) 本発明の一実施例を第3図から第8図において説明する
(One Embodiment of the Present Invention) One embodiment of the present invention will be described with reference to FIGS. 3 to 8.

本発明に係る車両用交流発電機の基本的構成は従来のも
のと同様である。第3図は固定子の磁極と回転子の磁極
歯部との相対的位置関係を示ず。
The basic structure of the vehicle alternator according to the present invention is the same as that of the conventional one. FIG. 3 does not show the relative positional relationship between the magnetic poles of the stator and the magnetic pole teeth of the rotor.

第3図において、τは回転子の磁極ピッチを示1゜(4
は回転子の磁4〜南部の底辺の長さを承り。底辺の長さ
(4はほぼ14ζ3τである。
In Fig. 3, τ indicates the magnetic pole pitch of the rotor, which is 1° (4
Accepts the length of the bottom of the rotor magnet 4~south. The length of the base (4 is approximately 14ζ3τ.

第4図(a)I3にび(I))は磁極南部の正面および
上面を示づ。磁極歯部20は所定の半径(約5uun以
上)を右するほぼ円弧状先端部21を有する。円弧状先
端部21の前面の長さ(lは(1′:τである。円弧状
先端部21の円弧の長ざβ2はほぼβ2’;2τである
。円弧状先端部21の底面の長さ13はJt3ζ5/2
τである。円弧状先端部21に連続してほぼ台形状の裾
野部22が形成される。台形状の裾野部22の上辺の長
さはjt3(”:5/2τ)で底辺の艮ざは14(ζ3
τ)である。台形状裾野部22の両側辺には所定角度θ
1 (約5°)をつけた一対の面取り部25が形成され
る。これらの面取り部25に連続して磁極円板部30に
その半径方向に沿って一対の而取り部35がざらに形成
されている。
FIG. 4(a) and (I)) show the front and top surfaces of the southern part of the magnetic pole. The magnetic pole tooth portion 20 has a substantially arcuate tip portion 21 extending at a predetermined radius (approximately 5 uun or more). The length of the front surface of the arc-shaped tip 21 (l is (1': τ). The length β2 of the arc of the arc-shaped tip 21 is approximately β2'; 2τ. The length of the bottom surface of the arc-shaped tip 21 is Sa13 is Jt3ζ5/2
It is τ. A substantially trapezoidal base portion 22 is formed continuously from the arcuate tip portion 21 . The length of the upper side of the trapezoidal base 22 is jt3 ('': 5/2τ), and the length of the base is 14 (ζ3
τ). A predetermined angle θ is formed on both sides of the trapezoidal base portion 22.
A pair of chamfered portions 25 with an angle of 1 (approximately 5°) are formed. Continuing from these chamfers 25, a pair of chamfers 35 are roughly formed in the magnetic pole disc part 30 along its radial direction.

面取り部35はそれぞれ所定の角度 θ2(0〈θ2〈45°)で形成される。(但しθ2=
θ −θ8−θC)円弧状先端部21の前而の両端から
台形状裾野部22の底辺の両端を結ぶ直線に沿ってつば
部26が形成される。磁極歯部20は側面28を有する
The chamfered portions 35 are each formed at a predetermined angle θ2 (0<θ2<45°). (However, θ2=
θ −θ8−θC) A collar portion 26 is formed along a straight line connecting both ends of the front end of the arcuate tip portion 21 to both ends of the bottom side of the trapezoidal base portion 22. The pole tooth 20 has a side surface 28 .

第5図(a )は第4図(a )のA−A’から見た磁
極歯部20の横断面図、第5図(b )は第4図(a 
)の3 3′から見た磁極円板81I35の横断面図お
よび第5図(C)は第4図(a )のC−C′から見た
磁極円板部35の横断面図である。
5(a) is a cross-sectional view of the magnetic pole tooth portion 20 seen from AA' in FIG. 4(a), and FIG.
) is a cross-sectional view of the magnetic pole disk portion 81I35 as viewed from 33', and FIG. 5(C) is a cross-sectional view of the magnetic pole disk portion 35 as viewed from CC' in FIG. 4(a).

第5図(a )、(b)、(c)に示された面取り部3
5に示された面取り角度θA10B、θCは而取り部3
5の面取り角度θ2に等しい。第6図(d )は第4図
(b)のD−D’ の、づ゛なゎち磁極歯部20の円弧
状先端部21の円弧の長さβ2にJ3りる縦断面を示す
。第6図(e )は第4図(b)のE−E’ における
、すなわち円弧状先端部21と裾野部22の接合部分に
お(プる縦断面を示ず。第6図<r>は第4図<b)の
F−F’a++分、すなわち裾野1(22と磁極円板部
3oとの接合部分にお【プる縦断面を丞す。第6図(d
 )、(e)、(f )に示される磁極歯部20の中心
Il’l11と側面28とが作る角度OD、θE、θ1
..は1゛べてθ。=θ、−〇、、、 −25°である
Chamfered portion 3 shown in FIGS. 5(a), (b), and (c)
The chamfer angles θA10B and θC shown in 5 are the chamfered portion 3.
It is equal to the chamfer angle θ2 of 5. FIG. 6(d) shows a vertical cross section taken along line DD' in FIG. 4(b), which is J3 along the arc length β2 of the arcuate tip portion 21 of the magnetic pole tooth portion 20. FIG. 6(e) does not show a vertical cross-section taken along line E-E' in FIG. 4(b), that is, the joint portion of the arcuate tip portion 21 and the base portion 22. represents the vertical cross-section extending from F-F'a++ in Fig. 4<b), that is, the joining part between the base 1 (22 and the magnetic pole disk portion 3o). Fig. 6(d)
), (e), (f) The angles OD, θE, θ1 formed by the center Il'l11 of the magnetic pole tooth portion 20 and the side surface 28
.. .. is 1 and θ. =θ, −〇, , −25°.

第4図(a )、(1))に示す面取り部25の作用を
従来技術との対比にJ3いて説明づる。従来のものは回
転子磁(41と、固定子磁極との回転相互位動関係によ
り、例λば回転磁極上の1点90(第1図(b)および
第11図参照)と対向異種の対応する回転磁極上の点9
0′とは、ある単一の固定子歯状磁極直下に位置する時
が存在する。この時、点80から点90′への磁気ボデ
ンシャル差に基づいて流れるili dWt&束通路に
関して該固定子磁極が第13〜14図に示’(9J+ 
<近接橋浪しづるので相当低パーミアンス(空隙長2ヶ
分のみ)となり当該固定子鉄心を経る、コイルに鎖交し
ない著しい漏洩磁束が発生ずる。そしてこの際漏洩磁束
が過大である為、当該固定子鉄心磁極先端部は飽和して
、本来の有効磁束をも阻み、また過大な漏哉磁束の為、
回転子異vA極面間の磁気ポテンシャル差も嗜゛分緩和
してこれまた本来の有効磁束を低めていた。第4図(a
)、(b)に示す如く面取り部25を設けることにより
前記磁束漏洩通路のパーミアンスが下がり、漏洩磁束は
激減し、前記問題は解消する。なおこの面取り部25は
、その角度θ1が急であったり、非面取り611の極弧
長!!3が小さかったりすると、磁気音が大きくなった
り固定子・回転子磁極間の平均空隙長増加の彫りの方が
大きくなり発生出力の低下につながることが考えられる
。どころか本実施例の如く磁極巾柔4(第3図)を(4
職3τ、J3(=5/2τ)−2,5τ、θ1−5°に
選ぶと固定子鉄心を経る漏洩磁束の低減効果を除外して
も空隙長の除々に変化する度合が滑らかなこと、および
横軸起磁ノコに対してパーミアンスが下がることによる
横軸反作用軽減の効果とにより磁気音、発生出力ともに
従来のものと同等以上であることがWI認されたーまた
第4図(b)に示J如く円弧状先端部?Xf 815の
角(第1図(a )、(11>で云えば4の箇所)を曲
線状に形成すると共に、第5図に示す如く、磁極ディス
ク部30(第7図参照)のうち反界磁コイル側の一部を
面取り部35としているので、従来大mに漏れでいた第
2N中φlb にて示す漏洩磁束はその通路のパーミア
ンスが低下して大巾に減る。なお、かくの如き面取り3
5はその内部の磁束通路断面積を縮小するので磁気回路
として不適当と考えられるかし知れないが、事実は、磁
束は大部分界磁コイル側を集中して流れるので、反界磁
コイル側は切除しても性能上人差ないことが判明してい
る。さらに、第6図に示1如く磁極側面28をθD′、
01.:X−0F 岬25°として、Jなわち相隣り合
う磁(船側面間の平均磁路長を拡大しパーミアンスを低
下さけているからこの箇所での漏洩磁束φ 、φ (第
2図参照)も大巾7a Ilc に減っている。
The function of the chamfered portion 25 shown in FIGS. 4(a) and (1)) will be explained using J3 in comparison with the prior art. In the conventional type, due to the mutual rotational positional relationship between the rotor magnetic poles (41) and the stator magnetic poles, for example, one point 90 on the rotating magnetic poles (see Fig. 1(b) and Fig. 11) and the opposite Point 9 on the corresponding rotating magnetic pole
0' means a time when the position is directly below a certain single stator tooth-shaped magnetic pole. At this time, the stator magnetic poles are shown in FIGS.
<Since the bridge wave is in close proximity, the permeance is quite low (only 2 air gap lengths), and significant leakage magnetic flux that does not link to the coil is generated through the stator core. At this time, since the leakage magnetic flux is excessive, the tip of the stator core magnetic pole becomes saturated, blocking the original effective magnetic flux, and due to the excessive leakage magnetic flux,
The magnetic potential difference between the different vA pole faces of the rotor was also somewhat relaxed, which also lowered the original effective magnetic flux. Figure 4 (a
By providing the chamfered portion 25 as shown in ) and (b), the permeance of the magnetic flux leakage path is lowered, the leakage magnetic flux is drastically reduced, and the above problem is solved. Note that the angle θ1 of this chamfered portion 25 may be steep, or the arc length of the non-chamfered portion 611 may be steep! ! If 3 is small, it is conceivable that the magnetic noise will become louder and the increase in the average gap length between the stator and rotor magnetic poles will become larger, leading to a decrease in the generated output. On the contrary, as in this embodiment, the magnetic pole width 4 (Fig. 3) is
When J3τ, J3(=5/2τ)-2,5τ, and θ1-5° are selected, the degree of gradual change in the air gap length is smooth even if the effect of reducing leakage magnetic flux through the stator core is excluded; WI confirmed that both the magnetic sound and generated output were equal to or higher than the conventional one due to the effect of reducing the horizontal axis reaction due to the lower permeance with respect to the horizontal axis magnetomotive saw. Also, Fig. 4 (b) Is the tip shaped like an arc as shown in J? The corner of Xf 815 (FIG. 1(a), (point 4 in 11>)) is formed into a curved shape, and as shown in FIG. Since a part of the field coil side is chamfered 35, the leakage magnetic flux shown at φlb in the second N, which conventionally leaked to a large amount m, is greatly reduced by reducing the permeance of the passage. Chamfer 3
5 may be considered inappropriate as a magnetic circuit because it reduces the cross-sectional area of the internal magnetic flux path, but the fact is that most of the magnetic flux flows concentrated on the field coil side, so It has been found that there is no difference in performance between people even if it is removed. Furthermore, as shown in FIG. 6, the magnetic pole side surface 28 is θD',
01. :X-0F Assuming the cape is 25 degrees, J, that is, adjacent magnetic fields (the average magnetic path length between the sides of the ship is expanded to avoid a decrease in permeance, so the leakage magnetic flux at this point φ, φ (see Figure 2) The width has also been reduced to 7a Ilc.

以上の如く具体的に各々の部分の漏洩パーミアンスを全
体として均等に低下させたから、大きな負荷電流が流れ
て、それに伴って第7図磁極面積20を拡大したことの
副作用としての大きな電機子反作用が働いても、前記米
国特許にみるような先行技術での欠点としてのとりわけ
負荷時に増大づる漏洩磁束の問題は解消する。
As mentioned above, since the leakage permeance of each part is specifically reduced uniformly as a whole, a large load current flows, and a large armature reaction occurs as a side effect of enlarging the magnetic pole area 20 in Fig. 7. However, the drawbacks of the prior art, such as that of the above-mentioned US patent, are overcome, especially the problem of increased leakage flux under load.

本発明を適用した回転子を12V80Aクラスの車両用
交流発電機につき同一の固定子、ハウジングを用いて、
同一励磁アンペアターンで、従来構成のものと発生出力
を比較したところ、従来一般の台形状ランゾル型磁極回
転子のものに対して全負荷状fF:4にd5い−C出力
が約7%、また前記米国特許3,004,181にみる
ような4図爪の回転子に対して約6%もの著しい出方向
上効果がみとめられた。前記実施例では第5図に示J如
くボールコアディスク部を35に示す如く断面を直線状
に面取りしているが、第8図に示す如く曲面状に而取り
しても回等の効果が得られる。また前記実施例では第6
図に示ずvA4!lii側面28の角反θつ、0 、θ
 をθD→θEζθF′、25°に選定しり、F ているが、θ、〉θE’=25’ >θ2に選定しても
よい。すなわら、磁極先暢:部稈、相隣り合う異磁極間
で第6図あるいは第10図80.80’ に相当すると
ころの爪状部失血相互の、或は爪状部先端はど磁路が飽
和するので、爪先端部と、第7図に示すところの、対向
する異極の谷間部30どの漏洩パーミアンスが減りかつ
、■極中実部、づなわち磁路断面積は磁1う−の根元楔
入きくとれて、磁気回路としてより適当であることは明
らかである。
A rotor to which the present invention is applied is used in a 12V80A class vehicle alternator using the same stator and housing.
Comparing the generated output with that of a conventional configuration with the same excitation ampere turn, the full load fF:4 to d5-C output was approximately 7% compared to that of a conventional general trapezoidal Ransol type magnetic pole rotor. In addition, a remarkable effect on the output direction of about 6% was observed for a rotor with four claws as seen in the above-mentioned US Pat. No. 3,004,181. In the above embodiment, as shown in FIG. 5, the cross section of the ball core disk part is chamfered in a straight line as shown in 35, but even if it is chamfered in a curved shape as shown in FIG. can get. Further, in the above embodiment, the sixth
Not shown in the diagram vA4! lii Angle anti-θ of side surface 28, 0, θ
is selected as θD→θEζθF', 25°, and F, but it may also be selected as θ,>θE'=25'>θ2. In other words, magnetic pole tip: between the culms and adjacent different magnetic poles, the blood loss of the claws corresponds to 80.80' in Fig. 6 or Fig. 10, or the tip of the claws is magnetic. Since the path is saturated, the leakage permeance at the tip of the claw and the opposing valley portion 30 of different polarities shown in FIG. 7 decreases, and It is clear that since the wedge can be removed from the base of the tube, it is more suitable as a magnetic circuit.

る。Ru.

(本発明の効駅) 以上述べたように本発明におい−Cは、磁極南部がそれ
ぞれ所定の半径を右する円弧状先端部を有し、磁極円板
部がぞれぞれ前記磁極歯部の両側に隣接配置された対向
異極のvA磁極歯部先端部に対応づる前記磁極円板部の
半径方向に一対の実質的面取り部35を有して成るので
、回転子の磁極先端部から円板部の対向S′1極への漏
洩磁束を低減できる効果かある。
(Effects of the Present Invention) As described above, in the present invention, the magnetic pole south part has an arc-shaped tip portion having a predetermined radius, and each of the magnetic pole disk portions has a circular tip portion that is located at a predetermined radius. Since the magnetic pole disk portion has a pair of substantial chamfered portions 35 in the radial direction corresponding to the tip portions of the vA magnetic pole teeth of opposite polarities adjacent to each other on both sides of the This has the effect of reducing leakage magnetic flux to the opposite pole S'1 of the disk portion.

本発明においてはさらに前記!i磁極山部前記磁極先端
部から実質的にテーパ状をなす裾野部を有しかつ前記先
端部および裾野部に関してほぼ台形状の断面を右づるの
で、回転子の磁極側面間の漏洩磁束の低減を図ることが
できる効果がある。
In the present invention, the above! i-Magnetic pole mountain portion Since the magnetic pole peak portion has a base portion that is substantially tapered from the magnetic pole tip portion, and the approximately trapezoidal cross section is tilted to the right with respect to the tip portion and the base portion, leakage magnetic flux between the sides of the magnetic poles of the rotor is reduced. This has the effect of making it possible to achieve this goal.

本発明はさらに、前記磁極山部はそれぞれ前記裾野部の
両側にその軸方向に治って形成された一対の面取り部2
5を有して成るから、回転子の磁極側面間の漏洩磁束を
さらに低減できる効果がある。
The present invention further provides that each of the magnetic pole mountain portions has a pair of chamfered portions 2 formed on both sides of the base portion in an axial direction.
5, it has the effect of further reducing leakage magnetic flux between the sides of the magnetic poles of the rotor.

【図面の簡単な説明】[Brief explanation of drawings]

第1図(a)i15よび(b)は従メこの交流発電機の
回転子の磁極歯部の正面図および上面図、第2図は従来
の交流発電(幾の回転子d5よび固定子部分を示づ図、
第3図は本発明一実施例に係る交流発電機の固定子磁極
と回転子歯部との相対的位置関係を示づ図、第4図(a
>および(b)は前記本発明一実施例の回転子の磁極南
部の正面図および上面図、第5図(a )〜(c)は第
4図(a)のA−A’ 、B−13’ 11;よびc−
c’ のそれぞれにおける横断面図、第(1図(d)、
(0)j5よび([)は第4図(1+)のl) D’ 
、 E−E’ J5よびF −F ’のそれぞれにおけ
る縦断面図、第7図は前記本発明一実施例の同り’A子
部分を示1図、第8図は本発明に係る他の実施例の回転
子磁極南部の横断面を示す図、負′19図は従来のつば
無し形状のボールコアを有する回転子の部分41?J造
を示J図、第10図は第9図をP方向から見た磁極歯部
を示す図、第11図は第10図をQh向から見たl1i
l極歯部を示す図、第12図は第11図のD−D’ に
お(プる断面図、第1:3図は従来の回転子磁極間で生
ずる近接橋渡しに31、る漏洩磁束を示1図、および第
14図は第13図に+lj Uる近接橋渡し漏洩磁束が
生ずるときの固定子ど回転子の位置関係を承り図である
。 1・・・tin極円極部 板部・・・磁極歯部 21・・・円弧状先端部 22・・・裾野部 25.35・・・而取り部 26・・・つば部 代理人 浅 村 皓 図面の浄書(内ig l−変更なし) 第 5 (¥1 第 6 図 牙7図 オ9図 第11図 才12図 才13図 牙14図 手続補正書(方式) 昭和5Z年ノ月、にに′日 特許庁長官殿 昭和6i年特許願aT θρ2/、≦“5号2、発明の
名称 女夙腋1鐵 36補正をする者 事件との関係 特許出願人 住 所 、貨 乱 日、)に電装林式会社 4、代理人 5、補正命令の日付 昭和42年 7月jノ日
Figures 1 (a) i15 and (b) are front and top views of the magnetic pole teeth of the rotor of this secondary alternating current generator, and Figure 2 is a conventional alternating current generator (rotor d5 and stator portion of A diagram showing
FIG. 3 is a diagram showing the relative positional relationship between stator magnetic poles and rotor teeth of an alternator according to an embodiment of the present invention, and FIG.
> and (b) are a front view and a top view of the southern part of the magnetic pole of the rotor according to the embodiment of the present invention, and FIGS. 5(a) to (c) are AA' and B- of FIG. 4(a). 13'11; and c-
Transverse cross-sectional views at each of c' (Fig. 1 (d),
(0)j5 and ([) are l in Figure 4 (1+)) D'
, E-E' J5 and F-F', FIG. 7 shows the 'A' part of the embodiment of the present invention, and FIG. A diagram showing a cross section of the southern part of the rotor magnetic pole of the embodiment, the negative diagram 19 is a portion 41 of the rotor having a conventional ball core without a flange. Figure 10 shows the magnetic pole tooth part as seen from the P direction in Figure 9. Figure 11 shows the l1i in Figure 10 seen from the Qh direction
Figure 12 is a cross-sectional view along line D-D' in Figure 11, and Figure 1:3 shows the leakage magnetic flux caused by proximity bridging that occurs between conventional rotor magnetic poles. 1 and 14 are diagrams showing the positional relationship between the stator and the rotor when the proximity bridging leakage magnetic flux of +lj U occurs in FIG. 13. 1...tin pole part plate part ... Magnetic pole tooth part 21 ... Arc-shaped tip part 22 ... Base part 25.35 ... Take part 26 ... Brim part Agent Ko Asamura Engraving of the drawing (including ig l - no changes) ) No. 5 (¥1 No. 6, Figure 7, Figure 9, Figure 11, Figure 12, Figure 13, Figure 14, Procedural Amendment (formula), November 1932, To the Commissioner of the Japanese Patent Office, 1939. Patent application aT θρ2/, ≦“5 No. 2, name of invention female armpit 1 iron 36 Relationship with the case Patent applicant address, currency Ran day,) Densorin Shiki Company 4, agent 5 , Date of amendment order: July j, 1962

Claims (1)

【特許請求の範囲】 (1) 対向配置された一対の磁極円板部と、前記円板
部の周辺部に相互に隔置されて設【プられた複数個の磁
極歯部であって各Il極歯部は円周方向につば部を有し
交互に反対極性で歯合された前記t41極山部とを有す
る回転子を含む交流発電(;父において、前記磁極歯部
はそれぞれ所定の半径を有づる円弧状先端部を有し、前
記磁極円板ff1llはそれぞれ前記磁極歯部の両側に
隣接配置された対向異極の磁極山部の先端部に対応する
前記磁極円板部の半径方向に一対の実質的面取り部(3
5)を有して成ることを特徴とりる交流発電機。 〈2、特許請求の範囲第1項記載の交流発電機において
、前記磁極山部は前記磁極先端部から実質的にテーパ状
をなす裾野部を有しかつ前記先端部d3よび裾野部に関
してほぼ台形状の断面をイコして成ることを特徴とする
交流発電機。 (3) 特許請求の範囲第2項に記載の交流光電機にお
いて、前記磁極山部はそれぞれ前記裾野部の両側にその
軸方向に沿って形成された一対の面取り部(25)を右
して成ることを特徴とづる交流発電機。
[Scope of Claims] (1) A pair of magnetic pole disk portions arranged opposite to each other, and a plurality of magnetic pole tooth portions provided at a distance from each other on the periphery of the disk portion, each of which The Il pole tooth portion has a collar portion in the circumferential direction, and the T41 pole tooth portion is alternately meshed with the opposite polarity. Each of the magnetic pole disks ff1ll has an arcuate tip portion having a radius, and each of the magnetic pole disks ff1ll has a radius of the magnetic pole disk portion corresponding to the tip portions of magnetic pole crest portions of opposite polarities disposed adjacently on both sides of the magnetic pole tooth portions. a pair of substantial chamfers (3
5) An alternating current generator characterized by comprising the following. <2. In the alternating current generator according to claim 1, the magnetic pole mountain portion has a base portion that is substantially tapered from the magnetic pole tip portion, and has an approximately base portion with respect to the tip portion d3 and the base portion. An alternating current generator characterized by having an equal cross section. (3) In the AC photoelectric machine according to claim 2, each of the magnetic pole peaks has a pair of chamfered portions (25) formed along the axial direction on both sides of the base portion. An alternating current generator characterized by:
JP20715383A 1983-11-04 1983-11-04 Ac generator Granted JPS6098854A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP20715383A JPS6098854A (en) 1983-11-04 1983-11-04 Ac generator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20715383A JPS6098854A (en) 1983-11-04 1983-11-04 Ac generator

Publications (2)

Publication Number Publication Date
JPS6098854A true JPS6098854A (en) 1985-06-01
JPH0564540B2 JPH0564540B2 (en) 1993-09-14

Family

ID=16535094

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20715383A Granted JPS6098854A (en) 1983-11-04 1983-11-04 Ac generator

Country Status (1)

Country Link
JP (1) JPS6098854A (en)

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63305741A (en) * 1987-06-08 1988-12-13 Mitsuba Electric Mfg Co Ltd Pawl shape of rotor core structure for automotive generator
JPS63305740A (en) * 1987-06-08 1988-12-13 Mitsuba Electric Mfg Co Ltd Rotor core structure for automotive generator
JPH02501973A (en) * 1987-02-11 1990-06-28 ローベルト ボツシユ ゲゼルシヤフト ミツト ベシユレンクテル ハフツング alternator with claw pole rotor
JP2003219617A (en) * 2002-01-21 2003-07-31 Mitsubishi Electric Corp Ac generator
JP2014128036A (en) * 2012-12-25 2014-07-07 Denso Corp Rotor of ac generator for vehicle
JP2016220513A (en) * 2015-05-15 2016-12-22 株式会社デンソー Vehicular rotary electrical machine
DE102018219339A1 (en) 2018-03-05 2019-09-05 Mitsubishi Electric Corporation ROTATING ELECTRIC MACHINE

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02501973A (en) * 1987-02-11 1990-06-28 ローベルト ボツシユ ゲゼルシヤフト ミツト ベシユレンクテル ハフツング alternator with claw pole rotor
JPS63305741A (en) * 1987-06-08 1988-12-13 Mitsuba Electric Mfg Co Ltd Pawl shape of rotor core structure for automotive generator
JPS63305740A (en) * 1987-06-08 1988-12-13 Mitsuba Electric Mfg Co Ltd Rotor core structure for automotive generator
JP2003219617A (en) * 2002-01-21 2003-07-31 Mitsubishi Electric Corp Ac generator
JP2014128036A (en) * 2012-12-25 2014-07-07 Denso Corp Rotor of ac generator for vehicle
US9755464B2 (en) 2012-12-25 2017-09-05 Denso Corporation Rotor for automotive alternator
JP2016220513A (en) * 2015-05-15 2016-12-22 株式会社デンソー Vehicular rotary electrical machine
DE102018219339A1 (en) 2018-03-05 2019-09-05 Mitsubishi Electric Corporation ROTATING ELECTRIC MACHINE
CN110233557A (en) * 2018-03-05 2019-09-13 三菱电机株式会社 Rotating electric machine

Also Published As

Publication number Publication date
JPH0564540B2 (en) 1993-09-14

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